260 Questions
Brownian motion each image frame is less than the displacement fluctuations in the
ABEL trap due to its finite stiffness? (Assume the room temperature viscosity of water
is 0.001 Pa⋅s.)
6.7
Assume solutions of the form A(ω) exp(iωt) for the Langevin force at angular fre
quency ω.
a
Derive an expression for the displacement x(t) at time t in an optical trap.
b
If the power spectral density G(ω)dω is defined as |A(ω)2|, derive an expression
for the mean squared displacement in terms of G.
c
Show that the power spectral density should be a Lorentzian function. (Assume
for “white noise” that G is a constant and that the equipartition theorem predicts
that the mean squared displacement at each separate frequency is associated with
a mean energy of kBT/2.)
6.8
An experimental protocol was devised using BFP detection to monitor the lateral dis
placement of a 200 nm diameter latex bead attached to a rotary molecular motor of
the bacterial flagellar motor (which enables bacteria to swim) via a stiff filament stub
to a live bacterium, which was free to rotate in a circle a short distance above the cell,
which itself is stuck firmly to a microscope coverslip. The motor is expected to rotate
at speeds of ~100 Hz and is made up of around ~20 individual subunits in a circle
that each are thought to generate torque independently to push the filament around.
a
What is the minimum sampling bandwidth of the QPD in order to see all of the
torque-generating units?
In practice, it is difficult to make a completely stiff filament; in a separate experi
ment using a completely unstiffened filament attached to a 500 nm diameter latex
bead, it was found that the filament compliance resulted in a relaxation drag delay to
bead movement following each ratchet of a few tenths of a microseconds, whereas
a 1000 nm diameter bead had an equivalent response time ~10 times slower.
b
Explain these observations and discuss which bead is the best choice to try to
monitor rotation mechanism of the flagellar motor.
It is possible to make some of the 20 ratchet subunits nonfunctional without
affecting the others.
c
How many subunits need to be made nonfunctional to detect individual activity
of each torque-generating subunit?
d
New evidence suggests that there may be cooperativity between the subunits—
how does this affect your previous answers?
6.9
AFM force spectroscopy and optical tweezers are both used to investigate single-
molecule mechanics stretching single biomolecules, as well as observing domain
unfolding and refolding of modules inside the molecules. Explain with reasoning if
one technique is better.
6.10 What is a “molecular signature,” and why are they needed? The “sawtooth” pattern
of a force-extension trace as obtained from AFM force spectroscopy on certain
molecules is an example of a molecular signature. Can you think of other molecular
signatures?
6.11 Single-molecule force spectroscopy is normally performed on purified molecules
or on the surface of cells. Why? Under what circumstances experiments might be
performed inside living cells?
6.12 At a prestigious biophysics tools and techniques awards dinner, a helium balloon
escaped and got loosely trapped just under the ceiling. Assuming no lateral friction,
how long would it take a red laser pointer of 1 mW power output to push the balloon
10 m across the length of the dinner hall ceiling using forward photon pressure alone?
How would this change using a fancier 5 mW green laser pointer? Would it make sig
nificant difference to encourage all the other ~500 people attending the awards dinner
to assist in getting out their laser pointers and performing this in parallel? (This is
what the author attempted in the not too distant past. It demonstrates the great merit
in doing theoretical calculations in advance of experiments.)
6.13 A membrane protein was imaged using AFM in contact mode. In one experiment, the
protein was purified and inserted into an artificial lipid bilayer on a flat surface. This